Estimation of the Lagrangian structure function constant C0 from surface-layer wind data

被引:23
作者
Anfossi, D [1 ]
Degrazia, G
Ferrero, E
Gryning, SE
Morselli, MG
Castelli, ST
机构
[1] CNR, Ist Cosmogeofis, I-10133 Turin, Italy
[2] Univ Fed Santa Maria, Santa Maria, RS, Brazil
[3] Univ Piemonte Orientale, Dip Sci Tecn Avanz, Alessandria, Italy
[4] ENEL SpA, SRI Area Ambiente, Milan, Italy
[5] Riso Natl Lab, DK-4000 Roskilde, Denmark
关键词
Lagrangian and Eulerian statistics; structure functions; autocorrelation functions; energy spectra; surface layer;
D O I
10.1023/A:1002697221093
中图分类号
P4 [大气科学(气象学)];
学科分类号
0706 ; 070601 ;
摘要
Eulerian turbulence observations, made in the surface layer under unstable conditions (z/L > 0), by a sonic anemometer were used to estimate the Lagrangian structure function constant C-0. Two methods were considered. The first one makes use of a relationship, widely used in the Lagrangian stochastic dispersion models, relating C-0 to the turbulent kinetic energy dissipation rate epsilon, wind velocity variance and Lagrangian decorrelation time. The second one employs a novel equation, connecting C-0 to the constant of the second-order Eulerian structure function. Before estimating C-0, the measurements were processed in order to discard non-stationary cases at least to a first approximation and cases in which local isotropy could not be assumed. The dissipation epsilon was estimated either from the best fit of the energy spectrum in the inertial subrange or from the best fit of the third-order longitudinal Eulerian structure function. The first method was preferred and applied to the subsequent part of the analysis. Both methods predict the partitioning of C-0 in different spatial components as a consequence of the directional dependence of the Eulerian correlation functions due to the isotropy. The C-0 values computed by both methods are presented and discussed. In conclusion, both methods provide realistic estimates of C-0 that compare well with previous estimations reported in the literature, even if a preference is to be attributed to the second method.
引用
收藏
页码:249 / 270
页数:22
相关论文
共 58 条
  • [1] ANAND MS, 1985, TURBULENT SHEAR FLOW, V4, P46
  • [2] ANGELL JK, 1971, Q J ROY METEOR SOC, V97, P87, DOI 10.1002/qj.49709741108
  • [3] [Anonymous], 1988, 8 S TURBULENCE DIFFU
  • [4] [Anonymous], 1959, ADV GEOPHYS VOL, DOI DOI 10.1016/S0065-2687(08)60122-3
  • [5] A STUDY OF THE ASSESSMENT OF AIR-TEMPERATURE, AND SENSIBLE-HEAT AND LATENT-HEAT FLUXES FROM SONIC-ANEMOMETER OBSERVATIONS
    CASSARDO, C
    SACCHETTI, D
    MORSELLI, MG
    ANFOSSI, D
    BRUSASCA, G
    LONGHETTO, A
    [J]. NUOVO CIMENTO DELLA SOCIETA ITALIANA DI FISICA C-GEOPHYSICS AND SPACE PHYSICS, 1995, 18 (04): : 419 - 440
  • [6] CORRSIN S, 1963, J ATMOS SCI, V20, P115, DOI 10.1175/1520-0469(1963)020<0115:EOTRBE>2.0.CO
  • [7] 2
  • [8] Csanady G.T., 1980, Turbulent Diffusion in the Environment
  • [9] Estimation of the Kolmogorov constant Co from classical statistical diffusion theory
    Degrazia, G
    Anfossi, D
    [J]. ATMOSPHERIC ENVIRONMENT, 1998, 32 (20) : 3611 - 3614
  • [10] ESTIMATION OF THE KOLMOGOROV CONSTANT (C-0) FOR THE LAGRANGIAN STRUCTURE-FUNCTION, USING A 2ND-ORDER LAGRANGIAN MODEL OF GRID TURBULENCE
    DU, SM
    SAWFORD, BL
    WILSON, JD
    WILSON, DJ
    [J]. PHYSICS OF FLUIDS, 1995, 7 (12) : 3083 - 3090